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Fluorescence lifetime imaging microscopy (FLIM) is a quantitative microscopy technique for imaging nanosecond decay times of fluorophores. In the case of frequency-domain FLIM, several methods have been described to resolve the relative abundance of two fluorescent species with different fluorescence decay times. Thus far, single-frequency FLIM methods generally have been limited to quantifying two species with monoexponential decay. However, multiexponential decays are the norm rather than the exception, especially for fluorescent proteins and biological samples. Here, we describe a novel method for determining the fractional contribution in each pixel of an image of a sample containing two (multiexponentially) decaying species using single-frequency FLIM. We demonstrate that this technique allows the unmixing of binary mixtures of two spectrally identical cyan or green fluorescent proteins, each with multiexponential decay. Furthermore, because of their spectral identity, quantitative images of the relative molecular abundance of these fluorescent proteins can be generated that are independent of the microscope light path. The method is rigorously tested using samples of known composition and applied to live cell microscopy using cells expressing multiple (multiexponentially decaying) fluorescent proteins.

Background: Wide-field frequency-domain fluorescence lifetime imaging microscopy (FLIM) is an established technique to determine fluorescence lifetimes. Disadvantage of wide-field imaging is that measurements are compromised by out-of-focus blur. Conventional scanning confocal typically means long acquisition times and more photo bleaching. An alternative is spinning-disc confocal whereby samples are scanned simultaneously by thousands of pinholes, resulting in a virtually instantaneous image with more than tenfold reduced photo bleaching., Methods: A spinning disc unit was integrated into an existing FLIM system. Measurements were made of fluorescent beads with a lifetime of 2.2 ns against a 5.3 ns fluorescent background outside the focal plane. In addition, living HeLa cells were imaged with different lifetimes in the cytosol and the plasma membrane., Results: In spinning-disc mode, a lifetime of the beads of 2.8 ns was measured, whereas in wide field a lifetime of 4.1 ns was measured. Lifetime contrast within living HeLa cells could be resolved with the spinning-disc unit, where this was impossible in wide field., Conclusions: Integration of a spinning-disc unit into a frequency-domain FLIM instrument considerably reduces artifacts, while maintaining the advantages of wide field. For FLIM on objects with 3D lifetime structure, spinning-disc is by far preferable over wide-field measurements., ((c) 2007 International Society for Analytical Cytology.)

Enhanced cyan and yellow fluorescent proteins are widely used for dual color imaging and protein-protein interaction studies based on fluorescence resonance energy transfer. Use of these fluorescent proteins can be limited by their thermosensitivity, dim fluorescence, and tendency for aggregation. Here we report the results of a site-directed mutagenesis approach to improve these fluorescent proteins. We created monomeric optimized variants of ECFP and EYFP, which fold faster and more efficiently at 37 degrees C and have superior solubility and brightness. Bacteria expressing SCFP3A were 9-fold brighter than those expressing ECFP and 1.2-fold brighter than bacteria expressing Cerulean. SCFP3A has an increased quantum yield (0.56) and fluorescence lifetime. Bacteria expressing SYFP2 were 12 times brighter than those expressing EYFP(Q69K) and almost 2-fold brighter than bacteria expressing Venus. In HeLa cells, the improvements were less pronounced; nonetheless, cells expressing SCFP3A and SYFP2 were both 1.5-fold brighter than cells expressing ECFP and EYFP(Q69K), respectively. The enhancements of SCFP3A and SYFP2 are most probably due to an increased intrinsic brightness (1.7-fold and 1.3-fold for purified recombinant proteins, compared to ECFP & EYFP(Q69K), respectively) and due to enhanced protein folding and maturation. The latter enhancements most significantly contribute to the increased fluorescent yield in bacteria whereas they appear less significant for mammalian cell systems. SCFP3A and SYFP2 make a superior donor-acceptor pair for fluorescence resonance energy transfer, because of the high quantum yield and increased lifetime of SCFP3A and the high extinction coefficient of SYFP2. Furthermore, SCFP1, a CFP variant with a short fluorescence lifetime but identical spectra compared to ECFP and SCFP3A, was characterized. Using the large lifetime difference between SCFP1 and SCFP3A enabled us to perform for the first time dual-lifetime imaging of spectrally identical fluorescent species in living cells.

Although the distribution of DNA-binding proteins inside the cell nucleus can be analyzed by immunolabeling or by tagging proteins with GFP, we cannot establish whether the protein is bound to DNA or not. Here, we describe a novel approach that allows imaging of the in situ interaction between a GFP-fusion protein and DNA in the cell nucleus, using fluorescence resonance energy transfer (FRET). We used fluorescence lifetime imaging microscopy (FLIM) as a reliable tool to detect protein in contact with DNA. The method was successfully applied to the DNA-binding proteins histone H2B and the glucocorticoid receptor and to the heterochromatin-associated proteins HP1alpha and HP1beta.

Fluorescence resonance energy transfer (FRET) is an extremely effective tool to detect molecular interaction at suboptical resolutions. One of the techniques for measuring FRET is acceptor photobleaching: the increase in donor fluorescence after complete acceptor photobleaching is a measure of the FRET efficiency. However, in wide-field microscopy, complete acceptor photobleaching is difficult due to the low excitation intensities. In addition, the method is sensitive to inadvertent donor bleaching, autofluorescence and bleed-through of excitation light. In the method introduced in this paper, donor and acceptor intensities are monitored continuously during acceptor photobleaching. Subsequently, curve fitting is used to determine the FRET efficiency. The method was demonstrated on cameleon (YC2.1), a FRET-based Ca(2+) indicator, and on a CFP-YFP fusion protein expressed in HeLa cells. FRET efficiency of cameleon in the presence of 1 mm Ca(2+) was 31 +/- 3%. In the absence of Ca(2+) a FRET efficiency of 15 +/- 2% was found. A FRET efficiency of 28% was found for the CFP-YFP fusion protein in HeLa cells. Advantages of the method are that it does not require complete acceptor photobleaching, it includes correction for spectral cross-talk, donor photobleaching and autofluorescence, and is relatively simple to use on a normal wide-field microscope.

Fluorescence lifetime imaging microscopy (FLIM) is a technique to map the spatial distribution of nanosecond excited state lifetimes within microscopic images. FLIM systems have been implemented both in the frequency domain, using sinusoidally intensity-modulated excitation light and modulated detectors, and in the time domain, using pulsed excitation sources and time-correlated or time-gated detection. In this review we describe the different modes in which both frequency-domain and time-domain FLIM instruments have been constructed in wide-field and in point-scanning (confocal) microscopes. Also, novel additional strategies for constructing FLIM-instruments are discussed. In addition to technical implementation, this chapter gives an overview of the application of FLIM in cell biological en biomedical studies. Especially for in situ protein-protein interaction studies using fluorescence resonance energy transfer (FRET), FLIM has proven to be a robust and established technique in modern cell biology. Other application areas, including usage of lifetime contrast for ion-imaging, quantitative imaging, tissue characterization and medical applications, are discussed.

Summary Multimode fluorescence resonance energy transfer (FRET) microscopy was applied to study the plasma membrane organization using different lipidated green fluorescent protein (GFP)-fusion proteins co-expressed in cowpea protoplasts. Cyan fluorescent protein (CFP) was fused to the hyper variable region of a small maize GTPase (ROP7) and yellow fluorescent protein (YFP) was fused to the N-myristoylation motif of the calcium-dependent protein kinase 1 (LeCPK1) of tomato. Upon co-expressing in cowpea protoplasts a perfect co-localization at the plasma membrane of the constructs was observed. Acceptor-photobleaching FRET microscopy indicated a FRET efficiency of 58% in protoplasts co-expressing CFP-Zm7hvr and myrLeCPK1-YFP, whereas no FRET was apparent in protoplasts co-expressing CFP-Zm7hvr and YFP. Fluorescence spectral imaging microscopy (FSPIM) revealed, upon excitation at 435 nm, strong YFP emission in the fluorescence spectra of the protoplasts expressing CFP-Zm7hvr and myrLeCPK1-YFP. Also, fluorescence lifetime imaging microscopy (FLIM) analysis indicated FRET because the CFP fluorescence lifetime of CFP-Zm7hvr was reduced in the presence of myrLeCPK1-YFP. A FRET fluorescence recovery after photobleaching (FRAP) analysis on a partially acceptor-bleached protoplast co-expressing CFP-Zm7hvr and myrLeCPK1-YFP revealed slow requenching of the CFP fluorescence in the acceptor-bleached area upon diffusion of unbleached acceptors into this area. The slow exchange of myrLeCPK1-YFP in the complex with CFP-Zm7hvr reflects a relatively high stability of the complex. Together, the FRET data suggest the existence of plasma membrane lipid microdomains in cowpea protoplasts.

Background: Photobleaching can lead to significant errors in frequency-domain fluorescence lifetime imaging microscopy (FLIM). Existing correction methods for photobleaching require additional recordings and processing time and can result in additional noise. A method is introduced that suppresses the effects of photobleaching without the need for extra recordings or processing., Methods: Existing bleach correction methods and the method introduced in this report whereby the recording order of the phases is permuted were compared using numerical simulations., Results: Certain orders were found to make measurements virtually insensitive to photobleaching. At 12 recordings, errors in measured phase and modulation depth decreased by a factor 512 and 393, respectively, compared to recordings using sequential recording order. The optimal order is independent of modulation depth, phase, and extent of photobleaching. Thus, the same order can be used for practically all situations. Application of the method in FLIM measurements of EYFP-transfected HeLa cells was found effectively to suppress photobleaching induced artifacts., Conclusions: In view of the ease of implementation, its inherent robustness, and the possibility to still apply existing correction methods afterward, there is no good reason not to use the permuted recording order presented in this report instead of a sequential order., (Copyright 2004 Wiley-Liss, Inc.)

In conventional wide-field frequency-domain fluorescence lifetime imaging microscopy (FLIM), excitation light is intensity-modulated at megahertz frequencies. Emitted fluorescence is recorded by a CCD camera through an image intensifier, which is modulated at the same frequency. From images recorded at various phase differences between excitation and intensifier gain modulation, the phase and modulation depth of the emitted light is obtained. The fluorescence lifetime is determined from the delay and the decrease in modulation depth of the emission relative to the excitation. A minimum of three images is required, but in this case measurements become susceptible to aliasing caused by the presence of higher harmonics. Taking more images to avoid this is not always possible owing to phototoxicity or movement. A method is introduced, phiFLIM, requiring only three recordings that is not susceptible to aliasing. The phase difference between the excitation and the intensifier is scanned over the entire 360 degrees range following a predefined phase profile, during which the image produced by the intensifier is integrated onto the CCD camera, yielding a single image. Three different images are produced following this procedure, each with a different phase profile. Measurements were performed with a conventional wide-field frequency-domain FLIM system based on an acousto-optic modulator for modulation of the excitation and a microchannel-plate image intensifier coupled to a CCD camera for the detection. By analysis of the harmonic content of measured signals it was found that the third harmonic was effectively the highest present. Using the conventional method with three recordings, phase errors due to aliasing of up to +/- 29 degrees and modulation depth errors of up to 30% were found. Errors in lifetimes of YFP-transfected HeLa cells were as high as 100%. With phiFLIM, using the same specimen and settings, systematic errors due to aliasing did not occur.

Background: It was found earlier that the difference in volume between unstained X- and Y-chromosome-bearing sperm heads could be detected using interference microscopy in visible light. This could be the basis for an alternative to the conventional method to sort X and Y sperm, which uses DNA staining and ultraviolet (UV)-excitation that may be harmful to sperm cells. A novel technique is introduced combining interferometry with flow cytometry., Materials and Methods: Interference optics were built into an existing flow cytometer/cell sorter and used to sort fresh unstained bull sperm cells on the basis of their head volume. Sorted fractions were stained with a DNA stain, and reanalyzed using the conventional method., Results: Purities between 60-66% were found in both X- and Y-enriched fractions. It was possible to sort up to 300 cells per second. The system was found to be less sensitive to the orientation of sperm cells than the conventional method., Conclusions: Interferometry can be combined with flow cytometry and used to obtain significantly enriched fractions of X- and Y-bearing sperm without staining and UV light. Sorting speeds and purities at this point, however, are much lower than with the conventional method., (Copyright 2002 Wiley-Liss, Inc.)

Volume-based sorting of X- and Y-chromosome-bearing sperm cells could be an interesting alternative to the existing technique based on DNA content. Advantages would be that DNA staining and ultraviolet excitation, used in the existing technique, could be avoided. To assess the possibilities and limitations of sperm-head volume as sorting criterion, achievable purity and yield are determined for bull sperm. Two important parameters in this respect are the magnitude of the volume difference and the biological variation within each (X or Y) population. Earlier, we established a difference in volume matching the difference in DNA content (3.8%) between X- and Y-bearing bull sperm heads by comparing thicknesses and areas of high numbers of pre-sorted X- and Y-bearing bull sperm heads by interference microscopy and subsequent image analysis. Unfortunately, despite the high number of measurements, a direct determination of biological variations was not possible due to an unknown contribution of instrumental variations. In this paper, we determine the contribution of instrumental errors by measuring a single sperm head, varying parameters such as location in the image, orientation angle, focusing etc., simulating the behavior of the measuring system. After correction, both for the instrumental variation, and for the fact that the original samples were not pure, biological variations in volume of 5.9 +/- 0.8% were found. Our results indicate that when 10% of the bull sperm are sorted on basis of their head volume, a theoretical enrichment of 80% could be achieved. Expected purity and yield are lower than what is standard for the existing technique. At the moment, a technique to physically separate X- and Y-bearing sperm cells based on volume is not available. However, for applications for which the potential hazards of DNA staining and UV excitation are problematic, the development of such technique should be considered.

Background: To investigate the possibilities of sperm head volume as a sorting criterion for gender preselection, we determined the magnitude of the difference in volume of X- and Y-chromosome-bearing bull sperm heads., Materials and Methods: Bovine sperm heads were sorted on the basis of their DNA content in X- and Y-chromosome-bearing fractions, using an existing flow-cytometric technique. Images of sperm heads of both populations were recorded using Differential Interference Contrast (DIC) microscopy. After reconstructing the DIC images, the area and the optical thickness of sperm heads of both populations were determined., Results: We found a difference in volume of X- and Y-bearing bovine sperm heads matching the difference in DNA content (3.5-4%)., Conclusions: Our findings indicate that volume can be used as a criterion to distinguish X- and Y-chromosome-bearing sperm, making development of a technique to sort X- and Y-chromosome-bearing sperm based on head volume theoretically possible. A strong advantage of such a technique over the existing technique based on DNA content would be that X- and Y-chromosome-bearing sperm cells could thus be sorted without subjecting them to any staining.

Recently a method was presented for reconstructing optical pathlength distributions (OPDs) from images of weak phase objects obtained by a conventional differential interference contrast (DIC) microscope. A potential application of this technique is the determination of the mass of biological objects: by integrating the optical pathlength over the projected surface of the image of an object, a measure of the dry mass, i.e. the total mass of all solid constituents present in the object, is obtained. To assess the possibilities of DIC microscopy for this application, simulations were performed on computer-generated DIC images of objects of various sizes, shapes and orientation angles. After reconstructing the OPDs from these images, the integrated optical pathlength of each of the test objects was determined, and compared with the expected results. The parameter settings used in the reconstruction algorithm were found to be very important in obtaining a reliable measurement. Using optimal parameter settings, errors in the integrated OPD could be limited to a few per cent for circular objects within the investigated size range. For non-circular objects, however, the orientation angle of the object relative to the lateral shift was found to influence the measured values. Ellipses with their long axes perpendicular to the shift direction had a significantly higher integrated OPD than ellipses orientated parallel to the shift. By adjusting the reconstruction parameters the effect could be limited, but complete elimination of the artefact was not possible within the parameter range investigated.

An image processing algorithm is presented to reconstruct optical pathlength distributions from images of nonabsorbing weak phase objects, obtained by a differential interference contrast (DIC) microscope, equipped with a charge-coupled device camera. The method is demonstrated on DIC images of transparent latex spheres and unstained bovine spermatozoa. The images were obtained with a wide-field DIC microscope, using monochromatic light. After image acquisition, the measured intensities were converted to pathlength differences. Filtering in the Fourier domain was applied to correct for the typical shadow-cast effect of DIC images. The filter was constructed using the lateral shift introduced in the microscope, and parameters describing the spectral distribution of the signal-to-noise ratio. By varying these parameters and looking at the resulting images, an appropriate setting for the filter parameters was found. In the reconstructed image each grey value represents the optical pathlength at that particular location, enabling quantitative analysis of object parameters using standard image processing techniques. The advantage of using interferometric techniques is that measurements can be done on transparent objects, without staining, enabling observations on living cells. Quantitative use of images obtained by a wide-field DIC microscope becomes possible with this technique, using relatively simple means.